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INSTRUCTION
MANUAL
LIQUID SCINTILLATION COUNTING SYSTEM WITH
8K MCA (USB) ALONG WITH PC
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NUCLEONIX
SYSTEMS PRIVATE LIMITED
N
TYPE : LS620
Plot No : 162 A & B, PHASE II, I.D.A.Cherlapally, Hyderabad - 500 051
Ph: 91-040-27263701, 32918055, 32914548 FAX : 27262146, e-mail : [email protected]
(or) [email protected], Website : www.nucleonix.com
File Name :
Date
:
LS620_Man
20-08-2013
Contents
Description
Pg.No.
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CHAPTER I
Introduction
CHAPTER II
Specifications
CHAPTER III
Block diagram & System Description
CHAPTER IV
Operating Procedure
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01-08
09-10
11-13
4.1. System Interconnections
14-14
4.2. Operating Instructions
15-21
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CHAPTER – I
1.
INTRODUCTION ON LIQUID SCINTILLATION & THEORY
Liquid scintillation counting (LSC)is an analytical technique,which measures activity of
radionuclide from the rate of light photons emitted by a radioactive sample dissolved in a
liquid scintillator. It is a powerful technique especially for detection and quantification of
low energy radionuclides as it enjoys advantage of 100% source detector geometry.
The manual provides the user the operating procedure and system details of the PC based
manual liquid scintillation counting system with USB interface developed in BARC .The
liquid scintillation counting system presented here is designed using advanced technology.
It is a computer controlled manually operated system for detecting even small amount of
beta and alpha radioactivity. It has wide range applications in biology, Medicine and
Environmental studies. The system has been fabricated for the quantitative estimation of
beta emitters like,h3,c14 and p32 .Usage of excellent quality high efficiency matched pair
of photomultiplier tubes, precision fast and slow chamber with preamplifiers,USB based
spectroscopy quality MCA , rugged manually operated sample chamber with lead shield
allow the system to offer high efficiency even for low energy beta emitters such as tritium
and also a very low background w ith ability to count radioactivity in bulk quantify of samples
one by one.
The instrument is highly reliable and incorporates several built in features such as
coincidence correction for low background. The USB bus interface of the MCA provides
an excellent connectivity with most of the new PCs and laptop computers. The LSC
application software provided, integrates with the hardware providing online display of
spectrum build up and measure of the activity of the sample.
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1.1 WHY LIQUID SCINTILLATION?
Most of the detectors used to measure ionizing radiation (such as alpha,beta,and gamma
radiation )are based on the ability of the radiation to ionize materials or to excite atoms
within materials. When excitation is followed by fluorescent de excitation the light emitted
can be converted into electric current by light sensitive devices e.g. PMTs scintillation
detectors are based on light emission. A small current is generated when production of
charge carriers (i/e ions electrons and holes )takes place between the charged electrodes
of detector. Detectors based on production of charge carriers are either gas filled ionization
chamber,proportional counters and GM counters in which charge carriers are produced
by ionization of a gas of solid usually semiconductor crystals. In latter case electrons and
holes are produced in pairs.
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Gas detectors use a defined gas cavity surrounded by wall whose inner surface is electrically
conducting and acts as one electrode and a second electrode (sometimes a central wire
or rod),which penetrates the gas volume and is electrically insulated from the conducting
wall.There is a voltage applied between the two electrodes. When ionizing radiation enters
a gas- filled detector it may interact directly in the gas and knock charged particles,such
as electrons,from the wall;these electron may enter the gas and also cause ionization.
When ionization of the gas occurs, the positive and negative ions are attracted towards
the negative and positive electrodes,respectively.
Gas detectors can respond to alpha,and gamma radiation . In order to detect alpha and
beta radiation the detector must be equipped with a sufficiently thin window to allow these
radiations to enter the gas. Alpha particles travel very short distance in materials (often
less than 100 micrometers in solid low- atomic – number materials ) so the window must
be quite thin,usually about 1/3 the thickness of a standard sheet of paper.
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Scintillation detectors on the other hand respond to energy absorption from ionizing radiation
by emitting light. The light is most often measured with a photo multiplier tube that converts
the light to an electronic pulse. These detectors may be either inorganic crystals or organic
compounds . All inorganic scintillators rely on the crystalline nature of the material for light
production and most have impurity atoms,with ionization potentials less than atoms of the
crystal, added as activators. Ionizing radiation may elevate electrons can migrate in the
conduction band and band to it valence band may also move and ionizes host atom that it
encounters. The impurity ions introduce trapping levels in the energy gap between the
valance and conduction bands. In brief,electrons may move into an excited level of the
activator ion and then drop to the ground energy state with the emission of light. Inorganic
crystalline scintillators, especially sodium iodide activated with thallium,NI (Tl),have been
mainly used for gamma-ray detection because of their high atomic number and thus a high
photoelectric cross section for gamma-rays.
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Scintillation detectors for beta radiation are often organic scintillators. Organic scintillators
operate at the molecular level, which means that the light emission occurs as a result of
fluorescence as a molecule relaxes from an excited level following excitation by energy
absorption from ionizing radiation . Molecules such as anthracene, trans-stilbene,
paraterphenyl,j and phenyl oxazole dervatives are among the many organic species that
have useful scintillation properties. Such organic molecules dissolved in organic solvents
are used as liquid scintillators. A classic application is in the measurement of low-energy
beta radiation (e.g., from tritium,c14,). In such cases the sample containing the radioactive
beta emitter is dissolved in, or in some cases suspended in, the liquid scintillation solution
.
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The emitted beta radiation transfers energy through the solvent to the scintillator
molecule,which then emits light that is detested by photomultiplier tubes . Liquid scintillators
can also be used for alpha particle measurements energy measurements. The key difference
is that in LSC the scintillation takes place in a solution of scintillator, rather than in a solid
crystal . This allows close contact between the isotope atoms and the scintillator, which is
not possible with solid scintillation .
With LSC the short path length of soft beta emission is not an obstacle to obstruction.
Thus though beta spectroscopy is possible with gas detector and solid state detectors
also but the advantage of 100% source detector geometry in the case of liquid scintillator
makes it the ideal detector choice especially for low energy beta emitters like tritium . Also
organic scintillators essentially contain carbon,hydrogen i.e low atomic number elements
resulting in less back scattering for beta radiations. All this goes to make liquid scintillation
detectors and ideal choice for beta as well as alpha emitters.
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1.2 THEORY OF LIQUID SCINTILLATION
Liquid scintillation counting is an analytical technique, which measures activity of
radionuclides from the rate of light photons emitted by a liquid sample. In this technique
the radioactive material (such as h3 , c14) is dissolved in liquid scintillation system consisting
of a solvent (such as toluene ) and a scintillating solute (such as PPO) contained in a glass
or plastic vial. The radiations emitted by the radioactive sample transfer energy to solvent
molecules,which get excited and transfer their energy to solute molecules, which on deexcitation emit photons. Some times a secondary solute is used to match the wavelength
of light emitted to that of PMT characteristics. The number of photons emitted is
proportional to energy of radiation and is detected using photo multiplier tubes and
associated electronic circuits.
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LIQUID SCINTILLATION PRINCIPLES
β
β
Radioactive materials
Excited Solvent Molecules
Fluor Molecule
Beta Particle
PMT
Analyzer
..
..... ..
The above figure provides a graphic illustration of the way the emitted radiation interacts
with the cocktail (a mixture of a solvent and a solute ) leading to a count being recorded
by the system.
The detailed stepwise procedure that results in emission of photons is given below.
3
a)
b)
c)
d)
e)
f)
Beta particle is emitted in a radioactive decay . To assured efficient transfer of energy of
its kinetic energy between the beta particle and the solution , the solution is a solvent for
the sample material.
In the relatively dense liquid, the beta particle travels only short distances before all of its
kinetic energy is dissipated. Typically a beta particle will take only a few nanoseconds to
dissipated all its kinetic energy. The energy is absorbed by the medium in 3 forms: heat,
ionization and excitation. Some of the beta energy is absorbed by solvent molecules making
them excited (not ionized).
Energy of the excited solvent is emitted as UV light and the solvent molecule returns to
ground state. The excited solvent molecules can transfer energy to each other and to the
solute . An excited solvent molecule,which passes its energy to a solute molecule,disturbs
the orbital electron cloud of the solute raising it to a state of excitation. As the excited
orbital electrons of the solute molecule return to the ground state, photon is emitted. If
photon is of UV light, an additional wavelength shifter is added which absorbs the UV
photon and emits blue light flashes upon return to ground state. Nuclear decay events
produce approximately 10 photons per keV of energy. The energy is dissipated in a period
of time on the order of 5 nanoseconds. The total number of photons from the excited solute
molecules constitutes the scintillation. The intensity of the light is proportional to the beta
particle’s initial energy.
Blue light flashes hit the photo cathode of the photo multiplier tube (PMT). Electrons
(proportional to the blue light pulses) are ejected producing an electrical pulses that is
proportional to the number of blue light photons. A LSC normally has two PMT’s the
amplitude of the PMT pulse depends on the location of the event within the vial . An event
producing 100 photons will be represented be a larger pulse if the event is closer to the
PMT than if the event is more remote . The signal from each PMT is fed into a circuit which
produces an output only if the 2 signals occur together, that is within the resolving time of
the circuit, approximately 20 nanoseconds(coincidence circuit ). By summing the amplitude
of the pulses from each PMT, an output is obtained which is proportional to the total intensity
of the scintillation. This analog pulse rises to its maximum amplitude and falls to zero.
The amplitude of the electrical pulse is converted into a digital value, which represents the
beta particle energy, passes into the analyzer where it is compared to digital value for
each of the L SC’s channels. Each channel is the address of a memory slot in a multichannel analyzer which consists of many storage slots or channels concentrating the energy
range from 0-1000keV .
In this manner, the sample is analyzed and the spectrum can be plotted to provide
information about the amount of radioactive material dissolved in the cocktail. The windows
based software provides on -line display of energy spectrum, total counts and elapsed
time of the sample along with set parameters display.
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1.3 FACTORS AFFECTING LIQUID SCINTILLATION COUNTING:
Following interferences are inherent to liquid scintillation process:
1.3.1 QUENCHING
The counting efficiency of the solute solvent system is affected by many different factors
which reduce detection efficiency. Some of the important processes are:
i) CHEMICAL QUENCHING:
Sosmetimes called impurity quenching causes energy losses in transfer from solvent
to solute.
ii) COLOR QUENCHING :
Energy losses occur when solution is colored, since photons when they pass through a
colored solution their wavelength may be altered to a value where PMT response is
reduced.
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1.3.2 CHEMICAL LUMINESCENCE/PHOTO LUMINESCENCE:
Chemical luminescence is production of light as a result of chemical reaction. This most
typically occurs in samples of alkaline pH and /or those containing peroxide, when mixed
with emulsifier-type scintillation cocktails.
Photo luminescence results in the activation of cocktail and /or vial by ultraviolet light or
cosmic rays in lab environment. Dark adaptation of one to two hour helps to decay all this
photo luminescence .
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1.3.3 ELECTROSTATIC DISCHARGE:
Electrostatic discharge is a photon producing interference in liquid scintillation counting.
Separation of two non conductive materials can generate significant amount of static
electricity. Static charges can develop in the scintillation vial or in scintillation cocktail, the
resulting discharge will produce light, which will be detected by a liquid scintillation counter.
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1.3.4 BACKGROUND:
For low level counting the lowest activity that can be measured is a function of background.
The factors causing background in a typical LSC system are:
a)
Instrument background:Results from the noise (Dark noise, after pulse noise) of
the PMT’s
b)
Cross talk: A scintillation event initiating photon within one PMT will be seen by the
other PMT
c)
Vial glass and PMT face:Background scintillation in the vial wall and the PMT face
are generated by the effects of cosmic or environmental radiation’s of glass walls
and PMT face (k40 radiation is present in glass wall and PMT face.)
d)
Scintillator: Scintillator background pulses are also caused by cosmic and
environmental radiation.
5
The first type of background is almost eliminated by using low nose matched pair of PMT’s
and by using a fast resolving circuitry. The signal from each PMT is fed into a circuit, which
produces an output only of the two signals arrive within a resolving time of 10-20 ns.
Vial glass containing a low k40 content should be chosen. Lead shielding is used to reduce
effect of cosmic radiations. All these factors result in a background of 12-15 cpm in tritium
window.
1.4.1 QUENCHING AND EFFICIENCY :
Quenching affects efficiency of conversion process beta particle energy to photo electron.
Therefore measured counts are only representative for the radio activity of the sample if
they are corrected for this quenching effect. All forms of quenching have the effect of reducing
the number of photons per keV of beta particle energy which reach the PMTs. Because
photons interact with PMT’s , the pulse amplitude is reduced for the same energy particle.
This result is a shift to lower amplitudes of the pulse height spectrum. For rsdionuclides
with high energy beta particles this shift may have little or no effect on counting efficiency
but with lower energy radionuclides the effect can be considerable. Tritium particularly is
affected by quenching. Because beta particle energy is co low that relatively few photons
are produced event with no quenching. With quenching a particle of higher energy will be
required to produce same number of photons. Events below coincidence threshold are
lost. Thus the collective effect of quench is a reduction in the number of photons produced
and, therefore, detected CPM( counts per minute). Counting efficiency is affected by the
degree is quenching in the sample. To determine absolute sample activity in DPM
(disintegration per minute or absolute activity), it is necessary to measure the level of
quench of the samples first, and then make the corrections for the measured reduction in
counting efficiency.
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Counting efficiency= CPM/DPM
1.4.2 MEASUREMENT OF QUENCH:
It is possible to measure quench accurately via high- resolution spectral analysis. Quenching
manifests itself by a shifting of the energy spectrum toward lower energy channels in the
multichannel analyzer(MCA)
To determine efficiency various methods as SCR (sample channel ratio), SIS( spectral
index of sample ) are used. The SIS value decreases as quench increases, reflecting the
shift of the spectrum to lower energy . each of these techniques involves measuring a set
of quenched standards all with the same activity but with different levels of quench. So
from the count rate obtained and efficiency calculated activity can be obtained.
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SIS = K
u
Σ X * n(x)
x=0
u
Σ n(x)
x=0
where : x is the channel number,
u is the end channel
n(x) is the counts at channel x
and K is a constant factor
1.4.3 QUENCH CURVE
A quench curve standard curve is a series of standards in which the absolute radioactivity
(DPM) per vial is constant and the amount of quench increases from vial to vial. A quench
curve uses the relation ship between counting efficiency and QIP (quench indicating
parameter ) (SCR&SIS are QIP) to correct the measured CPM to DPM . When a quench
curve is made, the DPM value in each standard is known. Each standard is counted and
the CPM is measured . The counting efficiency is calculated using the following relationship.
Counting efficiency= CPM/DPM
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At the same time, QIP is measured for each standard. A correlation is made using the QIP
on one axis (X) and the % efficiency on the other axis (Y). A curve is fitted to the standard
points. Once the quench curve is stored in the instrument computer, it can be used for
automatic DPM calculations. When unknowns are counted, the sample CPM and the QIP
are measured . Using the QIP , the counting efficiency is determined from the quench
curve. Sample DPM are then calculated by applying the appropriate efficiency to the
CPM of the sample.
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Efficiency
SIS
Efficiency correlation based on SIS
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Quenched spectrum
dN/dE
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Unquenched spectrum
Channel number
Effect of quenching on the accumulated spectrum
8
CHAPTER - II
SPECIFICATIONS
Detector
:
Cocktail consisting of radioactivity dissolved in liquid scintillator
contained in glass or plastic vial viewed by matched pair of
photo multiplier tube. PMT 9829 QA
Specifications of PMT 9829 QA : Two matched PMT power of E.T. make
Effective cathode size
:
45mm
Dynodes
:
12LFCsSb
Quantum efficiency
:
30%
Gain
:
6*106
Dark current
:
1 nano amp (typ)
Dark counts
:
200cps (typ)
V(k-a)
:
2800V (max)
I (a)
:
200 micro amp (max)
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Slow preamplifier(s)
:
One for each PMT are built-in. These two outputs are summed
& fed to MCA.
Fast pre-amplifier(s)
:
One for each PMT are built-in to check for time co-incidence
output to achieve low Background.
Housing
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Sample handling
:
Manually operated light sample chamber shielded with lead.
:
Using 20ml vials.
High Voltage Unit HV502 (TWO) : Two independently controllable HV are built-in with
(0-2000) [email protected] ripple & noise < 20mV.
Signal Proessing Unit SP560 : This is a two bit module, which received signals from slow/
fast pre-amplifier of each of the PMTs and processes the signal.
This essentially has coincidence circuit, summing amplifier and
shaping circuits. Output of this is fed to MCA card.
Output
:
Live display of acquisition of beta spectrum
9
Specifications of USB-MCA :
MCA resolution
Spectrum memory
Max counts / channel
Pulse processing time
Pile up rejection
DNL
INL
MCA Input
Timer
Preset Time
LLD, ULD, Baseline
Power requirement
:
:
:
:
:
:
:
:
:
:
:
:
256, 512, 1K, 2K, 4K and 8K channels
128 K bytes single port SRAM
31 bit (2 Giga counts)
7 ms including ADC conversion time of 5 ms
Active high TTL input from spectroscopy amplifier
Better than + 1%
Better than + 0.05% F.S
Single channel, 0 to +10 volts
32 bit, integrated in FPGA
LIVE or CLOCK, 1 sec to 136yrs
Digitally set through software
5V, ~ 500 mA through USB cable directly
(No external power supply required)
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Additional accessories required :
Personal Computer sytems :
(i) Unquenched standards
3
a. H 264200 DPM (typical)
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b. C 132400 DPM (typical)
c. Background
(ii) 20ml. sample vials for sample analysis
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Efficiency
:
(a) For tritium (3H) (in toluene based scintillating solution) >
50% with background less than 40 cpm
(b) For carbon (14C) (in toluene based scintillating solution) >
90% with background less than 70 cpm
Operating environment :
Air conditioned (20-25o) dust free environment.
Power
System operates on 230V, 50Hz, AC supply
High voltage : Auto set or user adjustable up to 1800V
:
10
CHAPTER - III
BLOCK DIAGRAM & SYSTEM DESCRIPTION
The manual Liquid Scintillation Counting System with USB interface consists of following
subsystems :
Sample chamber unit containing detector assembly having matched pair of photo multiplier
tubes with socket and pre-amplifiers.
This system consists of the following constituent unit
a. MINIM bin power supply (MB403),
b. High voltage modules (HV502 two numbers)
c. Signal Process unit (SP560),
d. USB MCA module
e. Sample chamber containing PMT’s with Lead shielding,
f. Personal Computer System
g. Unquenched standards (14C, 3H & Background)
h. Necessary inter connecting cables
The block diagram given below indicate inter connection between various sub-systems
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High Voltage Unit_1
HV502
(0-2000V)
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Slow Pre-amplifier 1
High Voltage Unit_2
HV502_2
Sample
(0-2000V)
Bottle
PMT
1
Fast Pre-amplifier 1
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PMT
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Sample chamber with
lead shield enclosure
Slow Pre-amplifier 2
Fast Pre-amplifier 2
Coincidence ckt
Shaping ckt
USB MCA
PC
Summing Amp
Signal processing unit (SP560)
LV (+12V)
LSC signal processing card
BIN & Power supply (MB403)
Low Voltages for Pre-amplfiers & High voltage units
Gating coincidence
output
11
LV (+12V)
The block diagram of manual PC based liquid scintillation counting system is shown above.
The system consists of a sample chamber that encloses a matched pair of photo multiplier
tubes. The photo multiplier tubes are mounted axially and view the scintillating solution contained
in a glass or plastic vial. The vial consists of the radioactive sample dissolved in the liquid
scintillation solution. The radiations emitted by the radioactive sample transfer energy to solvent
molecules, which get excited and transfer their energy to solute molecules, which on de-excitation
emit photons. Some times a secondary solute is used to match the wavelength of light emitted
to that of PMT characteristics. The light is emitted in duration of few nano seconds, as organic
scintillators are fast scintillators. The number of photons emitted is proportional to energy of
radiation and is detected by the two photo multiplier tubes. The response of the photomultiplier
tube to the photons incident on it is a current that flows for a time equal to charge collection time
as shown below. The time integral over the duration of the current is Q or the total amount of
charge generated in that specific interaction.
I(t)
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Time t
Pre-amplifiers mounted along with photo multiplier tubes process the electrical pulses
representing radioactive decay event from both the photo multiplier tubes.
The nature of the signal pulse produced from a single event depends on the input characteristics
of pre-amplifier to which the detector is connected. The equivalent circuit can be represented as
below.
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C
Detector
R
V
Here R represents input resistance of pre-amplifier and C represents equivalent capacitance of
detector, cable used to connect detector and input capacitance of pre-amplifier itself. If time
constant RC is kept very small in comparison to charge collection time then current flowing
through load resistance R is essentially equal to the instantaneous value of the current flowing in
detector. The signal voltage V under these conditions has a shape nearly identical to the time
dependence of the current produced within the detector.
This is case with fast pre-amplifier connected to photomultiplier in LSC system. The input
resistance R is kept 50 ohms. Fast pre-amplifier processes the current pulse from anode of
photomultiplier. The fast pre-amplifier output is negative analog voltage pulse of duration
approximately 20 nano secs. The signal pulse has a shape nearly identical to the time dependence
of the current produced within the detector.
12
If RC time constant is kept larger than detector charge collection time then detector current is
momentarily integrated on capacitance. The amplitude of signal pulse in this case is directly
proportional to the corresponding charge generated within detector.
This is case with slow pre-amplifier connected to photomultiplier in LSC system. R in this case
is kept in mega ohms, Thus output of slow pre-amplifier is proportional to the integrated charge
in detector. The amplitude of pulse of slow pre-amplifier output is thus proportional to charge
generated within detector or in other words proportional to energy of incident radiation. Also a
measurement of the rate at which such pulses occur will give the corresponding rate of radiation
interactions within detector.
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Thus fast and slow pre-amplifiers mounted along with photo multiplier tubes process the electrical pulses representing radioactive decay event from both the photo multiplier tubes. The fast
pre-amplifier as outlined above provides at its output a signal pulse that has a shape nearly
identical to the time dependence of the current produced within the detector (it is a fast linear
pulse of short duration approx 20 nano secs). The slow pre-amplifier as outlined above provides at its output a pulse whose amplitude is proportional to energy deposited in detector.
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The signals from the two fast pre-amplifiers are fed to LSC signal processing card. The LSC
signal processing card contains a coincidence circuit. This circuit produces an output only if the
two signals from the two fast pre-amplifier output occur together, that is within the resolving time
of the circuit, approximately 20 nano secs. Thus output of coincidence circuit on LSC signal
processing card is a TTL pulse that appears only when the pulses from the two fast pre-amplifiers arrive together. Noise pulses being random pulses thus do not result in a TTL pulse being
generated. This results in very low background. The signals from the two slow pre-amplifiers are
also fed to LSC signal processing card. The summation circuit present on LSC signal processing card is essentially a gated summation circuit. It sums only those pulses from the two slow
pre-amplifiers that arrive in coincidence. (Essentially the ON / OFF of gate is controlled by TTL
logic output of coincidence circuit). The coincident summed pulses are shaped by shaping circuit and fed to USB MCA card. In the MCA the amplitude of the pulse is converted into a digital
value, which represents the beta particle energy.
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In this manner, the sample is analyzed and the spectrum can be plotted to provide information
about the amount of radioactive material dissolved in the cocktail. The windows based software
provides online display of energy spectrum, total counts and elapsed time of the sample along
with set parameters display. The complete electronics i.e. high voltage required for photo multiplier tubes, low voltage, LSC signal processing card and USB based MCA are contained in a
single mains (230V) operated compact portable module.
13
CHAPTER - IV
INSTALLATION & OPERATING INSTRUCTIONS
Background
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(3C) 264200 DPM
(14C) 132400 DPM
Empty vial
Unquenched standards
4.1
SYSTEM INTER CONNECTIONS :
S.No
Name of the c able
From
To
1.
MHV to M HV co nnecto r
ca ble s (2 no’s)
Hig h volt age m od ule -1
Hig h volt age m od ule -2
HV1 of PMT1 (lef t side) B le ede r 1 (PM T)
HV2 of PMT2 (right side) B le eder 2 (PMT )
2.
BNC to B NC conn ector
ca ble s (5 no’s)
Fast Pre-am plifier -1
Slow P re -am plifie r 1
Fast Pre-am plifier-2
Slow P re -am plifie r-2
MC10 00U mod ule
F-IN1 F1 o f S P56 0
S-IN1 S o f S P56 0
F-IN2 F2 o f S P56 0
S-IN2 S2 of S P5 60
MCA m odule U SB of S P5 60
3.
9 pin D-t ype fem ale
co nnector t o 5 p in I/O
fem ale
MB 403 (B in rear sid e)
MB 403 (B in rear sid e)
Pre-am plifier -1
Pre-am plifier-2
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4.2. INSTALLATION PROCEDURE :
●
Unpack liquid scintillation counting system and place all the subsystems on the table. The
unpacked subsystems include the following units. (a) Minim Bin, (b) HV Module (c) Signal
Processing Unit, (d) USB MCA module, (e) Personnel Computer System with printer, (f)
Sample chamber with lead shielding, (g) Matched Photo multiplier tubes (PMT) (i) All
interconnecting cables etc.
●
Place the sample chamber with lead shielding arrangement in the middle of the table.
Demount cylindrical PMT housing shells and arrange to install the PMTs into this. Ensure
to open the PMTs from their packing in darkness.
●
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After installing them into cylindrical shell, close the sample chamber housing properly to
eliminate light leakage. Arrange bin with all these above modules plugged-in, along with
PC and printer as shown in the pi ctures on the front page of this user manual.
Make all the interconnection between various modules and sample chamber assembly as
per the details given in the interconnection table, under 4.1.
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Y
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P
●
Switch on the power to the instrument. Slowly increase the HV bias.
In the 2 HV modules (HV502) increase adj. dial till operating voltage, as specified for the
PMTs, has reached. (PMT manufacturer’s data has been taken into account) Important
Note : After loading of the PMT it may be good to leave the system overnight before using
the system. Next day only system can be powered-up for use.
●
To ascertain that the PMT housing and sample chamber has no light leakages, leave the
system for about 2 hours for background acquisition in PHA mode. User is requested to
ensure that the following unquenched standard and vials are kept ready for data acquisition
and standardization.
●
Now invoke MCA software and select PHA mode with 1K MCA channel (refer to MCA user
manual if required).
Now acquire the BG for 60 secs and they should not be any counts recorded without any
vial (BG/Standard) But it has been noticed that for 3H window (85-115) channel window
counts recorded were found to be 3 in 60 sec. for 14C window This indicates that there no
light leakages.
●
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15
Standards :
It is assured that the following standards are procured & are available for system calibration & installation
Pekin Elmer
Unquenched stadards (15ml)
Assay date : Aug 27, 2009
Expiration date : Aug 27, 2014
BG standard
H3 (Tritium) =
0.2µCi
262900
C14 (Carbon-14) = 0.1µCi
126700 DPM
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Next load Tritium (H-3) standard. Acquire PHA spectrum for about 60 sec. Now calculate
from this DPM and efficiency should be more or equal to 40%.
Screen dump of H3 (Tritum) PHA spectrum is shown in fig. (3)
Next replace BG standard and acquire the BG for 60 sec or 3 minutes. And compute BG,
but is has been that for 3H window (85-115) ----------------- 58 cpm. It should be less than or
equal 45 to 50%. in the (tritum) 3H RoI
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Substract the BG from standards. 14C & 3H
Efficiency calculation for (14C): CPM x 100
DPM
= 123251 x 100
132400
= 93.08%
X
I
N
O
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L
C
U
N
Efficiency calculation for (3H): CPM x 100
DPM
= 117558 x 100
264200
= 44.8%
Screen dump of BG for H3 PHA spectrum fig.(1)
Next replace Carbon (C-14) standard and count for 60 sec, calculate DPM and efficiency,
it should be equal or more that 90%.
Replace it with BG standard & count for BG for 60 sec with the same LLD & ULD settings.
Screen dump of C14 (carbon-14) PHA spectrum with standard fig.(4)
Calculate DPS & BG it should be less than 65 to 70%.
Screen dump of B.G for C14 fig.(2) in the (Carbon-14) 14C RoI, 90cpm.
Illustration of loading & unloading of standard(s) vails into PMT - sample chamber
assembly :
Fig. no. 5,6,7,10 & 11 clearly illustrates loading / unloading of vails into the chamber for
counting purposes.
16
S
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Fig (1) : B.G for H3 (PHA spectrum)
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Fig (2) : B.G for C14
17
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Fig(3) : H3 (Tritium) PHA spectrum (60-110) channels)
X
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C
U
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Fig (4) : C14 (Carbon-14) PHA spectrum with standardw
18
D
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Fig.5 : Liquid scintillation System PMT housing & sample chamber. Lever in ‘UP’ position
faciliates loading (place or remove) of ‘Vial’
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Once lever is rotated up then rotate vial chamber lid, in clockwise direction, and open the cap,
now vial, can either be placed or removed.
<
X
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C
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<
Rotate Vial holder in anti
clock direction.
Remove cap to load vial
either H3 or C14 standard for
counting.
Fig. 6
Now rotate vial holder in clock
wise complete as indicated &
slowly lower handle lever to
position the vial for counting
position.
>
Fig. 7
19
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Fig. 9 : Right side PMT connections
Fig. 8 : Left side PMT connections
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Lever ‘Down’ position vial counting
>
X
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C
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Fig. 10
Cap total clockwise position, facilitates
<
Lever ‘Up’ position
to load vial
>
Fig. 11
20
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<
Fig.13
T
V
P
Signal processing unit (SP560)
<
Fig.12
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C
U
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S
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S
Y
S
Fig.14 : USB - MCA module (MC1000U)
21